The axial and equatorial protons in cyclohexane can be distinguished by performing a variable-temperature NMR experiment. In this process, except for one proton, the remaining eleven protons are replaced by deuterium. The deuterium substitution avoids the possible peak splitting caused by the spin-spin coupling between the adjacent protons. The remaining proton flips between the axial and equatorial positions.
Figure 1. The temperature-dependent proton NMR spectra of cyclohexane.
Figure 1 depicts the proton NMR spectrum of the deuterium substituted sample, recorded at various temperatures. At room temperature, the rapid ring flipping of cyclohexane results in a single sharp peak. As the temperature is lowered to −60°C, the rate of chair-chair interconversion reduces, resulting in the broadening of the peak.
Further lowering of the temperature broadens the peak, forming a saddle that splits into two peaks. On reaching a temperature lower than −89°C, two sharp, well-resolved peaks corresponding to the equatorial and axial protons are formed. The peaks corresponding to the equatorial and axial protons occur at δ 1.62 and 1.14, respectively. At such low temperatures, the rate of chair-chair interconversion is reduced significantly, enabling the detection of the two distinct sets of protons on the NMR time scale.
The variable-temperature NMR technique helps distinguish between the two types of protons in cyclohexane - axial and equatorial.
To prevent the spin-spin coupling between the adjacent protons, eleven of the twelve protons are replaced by deuterium — the remaining proton switches between the axial and equatorial positions.
This sample is labeled cyclohexane-d11, and the corresponding proton NMR spectrum is recorded at various temperatures.
At room temperature, the rapid chair-chair interconversion produces a single sharp peak. However, the reduced rate at −60°C results in peak broadening. Further lowering of the temperature continues to broaden the peak — first, to form a saddle, which then splits into two peaks.
Below −89°C, two sharp, well-resolved peaks are formed at δ 1.62 and 1.14, corresponding to the equatorial and axial protons. At this temperature, NMR detects the two sets of protons due to the significantly low rate of chair-chair interconversion.